Volume 6: 5th International Conference on Multibody Systems, Nonlinear Dynamics, and Control, Parts A, B, and C 2005
DOI: 10.1115/detc2005-84917
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General Formulation of an Efficient Recursive Algorithm Based on Canonical Momenta for Forward Dynamics of Closed-Loop Multibody Systems

Abstract: In previous work, a method for establishing the equations of motion of open-loop multibody mechanisms was introduced. The proposed forward dynamics formulation resulted in a Hamiltonian set of 2n first order ODE’s in the generalized coordinates q and the canonical momenta p. These Hamiltonian equations were derived from a recursive Newton-Euler formulation. It was shown how an O(n) formulation could be obtained in the case of a serial structure with general joints. The amount of required arithmetical operation… Show more

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Cited by 7 publications
(10 citation statements)
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“…Particularly, if we define the SE(3) gradient of a function to be then we can apply this gradient to the parameters q = [q 1 , …, q 6 ] T used to parameterize a motion. Using (17) and observing that , we find that (18) This means that the inverse of the mass matrix for a single rigid-body can be written in the Fixman-like form: (19) For a collection of n rigid bodies, the configuration space is (SE (3)…”
Section: Extension To Chains Of Rigid Bodiesmentioning
confidence: 99%
See 2 more Smart Citations
“…Particularly, if we define the SE(3) gradient of a function to be then we can apply this gradient to the parameters q = [q 1 , …, q 6 ] T used to parameterize a motion. Using (17) and observing that , we find that (18) This means that the inverse of the mass matrix for a single rigid-body can be written in the Fixman-like form: (19) For a collection of n rigid bodies, the configuration space is (SE (3)…”
Section: Extension To Chains Of Rigid Bodiesmentioning
confidence: 99%
“…Hence, it differs from the direct sum of the inverse of Jacobian matrices, , where denotes the inverse Jacobian of the i th rigid-body. The inverse of the unconstrained mass matrix for this collection of rigid bodies is then of the form (20) Everything then follows using the extension of Fixman's theorem as in the point-mass case, with (20) replacing (4). The same partitioning into soft and hard variables and the same O(n) performance results.…”
Section: Extension To Chains Of Rigid Bodiesmentioning
confidence: 99%
See 1 more Smart Citation
“…A new, canonical momenta based algorithm was presented to solve the forward dynamics problem in a very efficient way, by reducing the number of operations required to obtain the equations of motion. It is also possible to handle constrained multibody systems with the algorithm, as shown in [15]. The purpose of this paper is to demonstrate some numerical examples and to point out some interesting features of the Hamiltonian equations related to the numerical integrations of these specific examples.…”
Section: Introductionmentioning
confidence: 99%
“…In previous publications [13,14], an attempt was made to address the first challenge. A new, canonical momenta based algorithm was presented to solve the forward dynamics problem in a very efficient way, by reducing the number of operations required to obtain the equations of motion.…”
Section: Introductionmentioning
confidence: 99%